Phenomenological and theoretical models for light baryon studies have been developed and modified over time. The light baryon resonances have been explored through well-known Isgur-Karl model basically applied for P-wave states [1]} as well as modified with relativised approach [2]}, Goldstone-boson exchange model due to spontaneous chiral symmetry breaking [3]}, [4]}, quark-diquark system along with Gursey-Radicati exchange intercation [5]}, [6]}, and semi-relativistic model with SU(6)-invariant and SU(6)-violating terms [7]}. Lately, varied approaches based on QCD SUM Rules [8]}, basis light-front model [9]} and light-front relativistic [10]}, Lattice QCD [11]} and covariant Faddeev approach [12]} and others based on n and \(J^{P}\)  values and the respective trajectories against square of mass of a given state. [13]}, [14]}. The spectrum of octet and decuplet light baryons has also been studied in a relativistic approach using instanton induced quark forces [15]}.
